Bearing, in particular for a magnetic levitation assembly

ABSTRACT

A magnetic bearing assembly ( 20 ) comprises a first magnet assembly ( 34 ) for generating a first quadrupole magnetic field in a first plane and a second magnet assembly ( 36 ) for generating a second quadrupole magnetic field in a second plane. The second plane is arranged parallel to the first plane. The quadrupole magnetic fields exhibit in each case in the planes magnetic field axes arranged at an angle to one another between four poles. A longitudinal axis (A) is defined at right angles hereto by the centres of the quadrupole magnetic fields. At least one diamagnetic element ( 44 ) is arranged on the longitudinal axis (A). The first and second magnet assemblies ( 34, 36 ) are arranged relative to one another in such a way that the first and the second quadrupole magnetic fields are rotated towards one another about the longitudinal axis (A) by an angular amount which is not a whole-number multiple of 90°. Such a bearing arrangement can be used in particular in a magnetic levitation assembly ( 10 ) with a lifting assembly ( 26 ).

RELATED APPLICATION(S)

This application is a continuation of U.S. patent application Ser. No.16/279,076 filed on Feb. 19, 2019 entitled “Bearing, in Particular for aMagnetic Levitation Assembly,” which is a continuation of U.S. patentapplication Ser. No. 15/763,554 filed on Mar. 27, 2018, subsequentlygranted as U.S. Pat. No. 10,218,294 issued on Feb. 26, 2019, entitled“Bearing, in Particular for a Magnetic Levitation Assembly,” which is aU.S. national stage application of International Patent Application No.PCT/EP16/73453 filed on Sep. 30, 2016, entitled “Bearing, in Particularfor a Magnetic Levitation Assembly,” which claims priority to GermanPatent Application No. 102015116767.0 filed on Oct. 2, 2015.

DESCRIPTION

The invention relates to a bearing assembly, magnetic levitationassembly, and a method for the bearing mounting of an axle element. Inparticular, the invention relates to a magnetic levitation assembly anddifferent aspects of magnetic levitation assemblies.

A magnetic levitation assembly as part of a magnetic levitation weighingscales device is disclosed, for example, in DE 10 2009 009 204 A1. Thisdiscloses a method and device for the levitation regulation of alevitation component, for example of a magnetic levitation weighingscales. The levitation component comprises a magnet element and aposition sensor. An electromagnet is actuated in such a way that itexercises a force effect on the magnet element.

WO 2007/065608 A1 describes a magnetic levitation system. A dipolemagnet is held in a two-dimensional or three-dimensional staticquadrupole magnetic field. In a preferred embodiment, a closed controlcircuit of a servosystem with anti-Helmholtz coils is formed, in whichthe current is measured, which is proportional to the mass. In thissituation, the dipole magnet is passive-stabilized by a diamagneticmaterial, which is embedded in a stabilizing magnetic field. Thestabilizing magnetic field in which the diamagnetic material is locatedis preferably a quadrupole field.

The object of the invention can be seen as providing a bearing assemblyand a method for the bearing mounting of an axle element, and a magneticlevitation assembly, with which good stabilization can be attained.

This object is solved according to a first aspect of the invention inaccordance with claim 1, a magnetic levitation assembly equipped withthis in accordance with claim 10, and a method for the bearing mountingof an axle element in accordance with claim 13. According to a secondaspect of the invention, the object is solved by a magnetic levitationassembly in accordance with claim 14. According to a third aspect of theinvention, the object is solved by a magnetic levitation assemblyaccording to claim 15. In this situation, the three aspects of theinvention are in each already advantageously ready for use alone, butare particularly suitable for combination.

With the bearing arrangement according to the invention and the methodaccording to the invention for the bearing mounting of an axle elementaccording to the first aspect of the invention, a first and a secondmagnet assembly are provided for the bearing mounting of a diamagneticelement on a longitudinal axis. The two magnet assemblies are in eachcase configured such as to produce quadrupole magnetic fields in firstand second planes assigned to them, i.e. the first magnet assemblygenerates a first quadrupole magnetic field in a first plane and thesecond magnet assembly generates a second quadrupole magnetic field in asecond plane. The first and second planes are arranged parallel to oneanother with a distance interval between them. A longitudinal axis, onwhich the diamagnetic element is arranged, runs at right angles to theplanes, through the centres of the quadrupole magnetic fields.

With this arrangement, a contact-free and therefore frictionlessmounting of the diamagnetic element by the quadrupole magnetic fieldscan be attained. Due to the diamagnetic properties, the diamagneticelement is centred on the longitudinal axis in the two quadrupolemagnetic fields, arranged longitudinally behind one another. Thediamagnetic element and each component located on this, such as an axle,shaft, levitation component, or another element, can therefore bemounted contact-free on the longitudinal axis. The mounting in thissituation allows for free movement in the longitudinal direction. Africtionless rotation about the longitudinal axis is also possible. Inparticular, the bearing mounting can be configured in such a way that noforces take effect on the diamagnetic element in the longitudinaldirection.

According to the invention, in this situation the first and secondmagnet assemblies are arranged relative to one another in such a waythat the first and the second quadrupole magnetic fields are rotated toone another. In this situation the angle of rotation is a multiple of90° which is not a whole number. The two quadrupole magnetic fields aretherefore arranged parallel to one another in the longitudinal axis, butare arranged rotated against one another.

With a quadrupole magnetic field, magnetic field axes are produced in aplane between the four poles which are arranged at an angle to oneanother. The rotation of the quadrupole magnetic fields about an anglewhich is a multiple of 90° which is not a whole number therefore leadsto an arrangement in which these magnetic field axes, seen in thelongitudinal direction, are not flush, but are offset to one another. Asa result, an especially good stabilizing of the dipole element isattained, the position of which, on the other hand, as the inventorshave determined, under certain circumstances cannot be adequatelystabilized in the direction of the magnetic field axes. Due to therotated arrangement, bearing forces are exerted in total on thediamagnetic element which do provide for good centring and stabilizingon the longitudinal axis.

While in principle this effect is already attained with every anglevalue of the rotation which is greater than 0° and is a multiple of 90°which is not a whole number, it has in practice proved favourable if therotation angular amounts, for example, to 5°-85°, preferably 10°-80°.With only two magnet assemblies, an angle of the rotation of 45°+/−20°or an odd-number multiple of these has proved especially favourable,since in that case the magnetic field axes of the quadrupole magneticfields arranged longitudinally next to one another stand at a maximumangle to one another, such that the stabilizing effect is particularlyperceptible. With more than two magnet assemblies arranged next to oneanother, angles of the rotation which are somewhat less are preferred,for example 10°-30°. With four magnet assemblies, for example, angles ofthe rotation of 10°-25° in each case are preferred.

Each magnet assembly can preferably be formed from a plurality ofmagnetic elements, for example of four or more, and preferably eight ormore individual magnetic elements. The magnetic elements are preferablypermanent magnetic elements. Preferably, in this situation magneticelements with radially and/or tangentially aligned magnetization areprovided, in order to generate the desired quadrupole magnetic field.For particular preference, the magnetization direction of the magneticelements is such that no components point in an axial direction.

In this situation, any magnetic assembly can preferably comprise aplurality of magnetic segment elements arranged around the longitudinalaxis. The magnetic segment elements can, for example, be arranged inring form around a free centre. In this situation, magnetic segmentelements are preferred which exhibit a trapezoidal form incross-section.

According to a further embodiment of the invention, magnetic segmentelements can be arranged in a Halbach array. With a Halbach array,segments of permanent magnets with different magnetic orientation arearranged directly next to one another in such a way that the magneticflux is intensified to one side. With the ring-form Halbach arraypreferred here, the magnetizing directions are arranged in the form of amagnetic orientation rotating along the ring, in such a way that themagnetic flux is intensified in the centre.

In the situation of the use of magnet assemblies with magnetic segmentelements, the rotation relative to one another can be attained, forexample, by a flush arrangement of magnetic segment elements of bothmagnet assemblies, but with magnetic orientation between the magnetassemblies deviating from one another. Such an arrangement can bestructurally simple. Preferably, the magnetic segment elements of bothmagnet assemblies are configured in such a way that they extend aroundthe longitudinal axis by an angle range which is of equal size in eachcase. The angular amount of the rotation can then correspond to awhole-figure multiple of the angle range of a magnetic segment. With onepreferred arrangement of, for example, eight magnetic segment elements,which in each case extend around the longitudinal axis over an anglerange of 45°, an offset of the magnet assemblies to one another by onemagnetic segment element results in a preferred angular amount of therotation of, for example, 45°.

By means of the at least two magnet assemblies provided for according tothe invention, an improved stabilizing of the diamagnetic elements isalready attained.

This can be improved still further in that, by means of a third magnetassembly, a third quadrupole magnetic field is generated in a thirdparallel plane, and, for further preference, by means of a fourth magnetassembly, a fourth quadrupole magnetic field is generated in a fourthparallel plane. It is also possible for further quadrupole magneticfields to be arranged along the longitudinal axis. In this situation,quadrupole magnetic fields which are preferably arranged next to oneanother along the axis are in each case rotated against one another byan angular amount which is a multiple of 90° which is not a wholenumber, even if it is already sufficient for the attaining of thestabilizing effect if such a rotation occurs between two magnetassemblies, preferably arranged at a distance from one another,regardless of the alignment of magnet assembles arranged in between.With three or more magnet assemblies, and also with four or more magnetassemblies, preferably all the magnet assemblies are rotated in eachcase in pairs about an angular amount which is a multiple of 90° whichis not a whole number. Accordingly, an offset is always provided betweenall magnetic field axes in the respective planes, such that thestabilizing effect is optimised.

The diamagnetic element can, for example, exhibit a cylindrical shape.In order to achieve weight savings, for example, it can be designed asshort, exhibiting a length, for example, which is less than the distanceinterval between the first and second planes. According to a furtherembodiment of the invention, however, it exhibits a length which isgreater than the distance interval between the first and second planes,i.e. the diamagnetic element extends along the longitudinal axis,through the planes of the two quadrupole magnetic fields. As a result,the situation can be attained that, even with a change of location inthe longitudinal direction, no forces, only the lowest forces possible,take effect in this direction. In the situation with additionallongitudinally-arranged quadrupole magnetic fields, it is furtherpreferred for the diamagnetic element to extend along the longitudinalaxis also through the respective parallel planes.

The bearing assembly described can be used in particular in a magneticlevitation assembly. In this situation, at least one first bearingassembly is provided for the mounting of a vertically orientedlevitation element, i.e. the longitudinal axis is aligned vertically andthe planes of the magnet assemblies are aligned horizontally.

The diamagnetic is located on the vertically extending levitationelement.

Further provided is at least one lifting assembly for the levitationelement. This comprises at least one lifting magnet element arranged atthe levitation element, preferably a permanent magnet element, which ismagnetised vertically, i.e. in the longitudinal direction of thelevitation element. The lifting assembly further comprises at least onelifting coil and/or one or more permanent magnet elements, in order togenerate a lifting magnetic field, by means of which a lifting force isgenerated which takes effect on the lifting magnet element, andtherefore on the levitation element.

The bearing assembly according to the invention is particularly wellsuited for use in such a magnetic levitation assembly. Due to the magnetassemblies taking effect horizontally, the levitation element isstabilized and centred in its vertical alignment. The bearing assemblycan preferably be configured in such a way that no force is generatedfrom this which takes effect in a vertical direction on the levitationelement.

The lifting force taking effect in the vertical direction can beregulated in such a way that the levitation element is held levitated,i.e. in a fixed position in the vertical direction. This can be attainedin particular by a regulation with a position sensor for the verticalposition of the levitation element, with which, for example, one or morelifting coils are subjected to current.

Such a magnetic levitation assembly can be used in particular formeasuring purposes, for example in a magnetic levitation weighing scalesfor measuring weight force, and therefore the mass of a sample takenfrom the levitation element, or for measuring other forces taking effecton the levitation element, which this experiences, for example, in aflowing medium.

Measurements, in particular of the weight force or of other forcestaking effect on the levitation element, can be carried out, forexample, by an external weighing cell, which is coupled to the liftingelements, i.e. to the lifting coil and/or the permanent magnet elements.Preferred, however, is a measurement of such forces by a measurement ofthe current through the lifting coil or coils.

In preferred embodiments, at least one lifting coil and/or at least onering-shaped permanent magnet are arranged around the levitation element.For particular preference, two lifting coils and/or ring magnets areprovided arranged axially at a distance from one another, between whichthe lifting magnet element is arranged. The lifting coils can inparticular be subjected to current as anti-Helmholtz coils, in order togenerate a suitable lifting magnetic field. Ring magnets are preferablymagnetized in axially opposed directions, such that, preferably, asimilar magnetic field to that of the lifting coils is generated. With ahybrid arrangement with lifting coils and permanent magnet elements, thefield portions are overlaid and amplified in a preferred manner.

According to a further embodiment of the invention, with a magneticlevitation assembly at a distance from the first magnetic bearingassembly, a second bearing assembly can also be provided for, in such away that the lifting assembly is arranged at least in part between thefirst and the second bearing assembly. In this way a preferablycontinuous levitation element can be well stabilized.

While in this situation the use of the special bearing assembliesaccording to the invention is preferred, with quadrupole magnetic fieldsrotated with one another, the arrangement of two magnetic bearings aboveand below the lifting assembly of a magnetic levitation assembly alreadyalso results in a stabilizing which is adequate for many purposes withthe use of single quadrupole magnet assemblies. Accordingly, this secondaspect of the invention according to claim 13 is also regarded asseparately advantageous independently of the use of special bearingassemblies.

In a further preferred embodiment of a magnetic levitation assembly, thelevitation element can be configured as a continuous rod of a ceramicmaterial. In this situation it is preferred for at least one diamagneticelement located on the levitation element and/or the lifting magnetelement provided at the levitation element to be configured in a ringshape, and to be arranged around the continuous rod. Such an arrangementhas proved to be particularly suitable. Preferably, all the elementsprovided at the levitation element which take effect electrically ormagnetically are configured in ring shape, and are arranged around acontinuous ceramic rod, in particular the diamagnetic element of atleast one first bearing assembly, and also the lifting magnetic element.For further preference, with the use of a second bearing, this alsoapplies to the second diamagnetic element, as well as to a part of aposition sensor arranged at the levitation element, such as an optical,electrical, or magnetic sensor.

This aspect of the structure of a magnetic levitation assembly doesindeed also offer particular advantages in combination with the specialbearing assembly according to the first aspect of the invention, andstabilizing by two bearings in accordance with the second aspect of theinvention, but it is already advantageous when considered on its own.This third aspect of the invention according to claim 14 can thereforealso be used independently of the special arrangement of the bearingassemblies according to the first aspect of the invention, and the useof two bearing assemblies arranged at a distance from one another inaccordance with the second aspect of the invention.

Exemplary embodiments of the invention are described in greater detailhereinafter on the basis of drawings. The drawings show:

FIG. 1 In a schematic representation, a longitudinal section through amagnetic levitation assembly of a magnetic levitation weighing scales;

FIG. 2 in a side view, a bearing assembly of the magnetic levitationassembly according to FIG. 1;

FIG. 3 a front view of a magnetic assembly of the bearing assembly fromFIG. 2;

FIG. 4 a schematic representation of a quadrupole magnetic field of themagnetic assembly from FIG. 3;

FIG. 5 a schematic exploded representation of two magnet assemblies;

FIGS. 6,7 in a schematic representation of longitudinal sections, afirst and a second embodiment of an arrangement for the measuring offlow forces.

FIG. 1 shows a longitudinal section through a magnetic levitationassembly 10. In this situation, the representation in FIG. 1 and in thefollowing figures is to be understood as schematic in each case, withthe aim of a clear understanding of the basic structure and of the mostimportant components of the assembly, wherein actual devices comprise aplurality of further elements, such as housings, etc. In particular, therepresentations are not to scale.

The magnetic levitation assembly 10 comprises a vertically alignedlevitation part 12, with a continuous longitudinal ceramic rod 14. Thelevitation part 12 is arranged freely levitating inside the stationaryelements, which are described in individual detail hereinafter. In thissituation, the magnetic levitation assembly 10 in the example shown isconfigured for use as a levitation weighing scales, with a sample takingdevice 16 under the casing represented by way of example, and a sampletaking device 18 above the casing. The use of the magnetic levitationassembly 12 as a levitation weighing scales represents only one example,however; the assembly described hereinafter can in fact also be used forother purposes.

The magnetic levitation assembly 10 comprises an upper bearing 20 and alower bearing 22, a position sensor 24, and a lifting assembly 26.

The lifting assembly 26 serves to hold the levitation part 12 in adesired vertical levitation position. For this purpose, its weight forceis compensated by a counteracting magnetic force. By means of the sensor24, the vertical position of the levitation part 12 is determined, suchthat the lifting assembly 26 can be regulated for the adjustment of thelevitation location. In the example shown, the sensor 24 is an inductivesensor, with which the setting of an index element 48 at the levitationpart 12 is determined contact-free, in relation to stationary sensorcoils.

In the example shown, the lifting assembly 26 comprises two liftingcoils 28, 30, which are arranged at a distance from one another,coaxially about the levitation element 12. Arranged between the liftingcoils 28, 30, at the levitation part 12 is a magnetic dipole element 32,as the lifting magnet element. The lifting magnet element 32 is aring-shaped permanent magnet element, arranged around the ceramic bar 14of the levitation part 12, which is magnetised in the longitudinaldirection of the levitation part 12.

The lifting coils 28, 30 are provided with a regulated current by anactuation device (not represented). In this situation they are connectedand switched as anti-Helmholtz coils, and therefore generate a liftingmagnetic field, which exerts a lifting force, counteracting the weightforce, on the lifting magnet element 32, and therefore on the levitationpart 12. The actuation device in this situation receives a positionsignal from the position sensor 24, and regulates the current throughthe lifting coils 28, 30 in such a way that a fixed levitation positionis adopted and held; i.e. the weight force is exactly compensated.

For use as a magnetic levitation weighing scales, the current can thenbe measured through the lifting coils 28, 30. This is proportional tothe weight force and therefore to the mass of the levitation part 12,such that the mass can be determined of the samples taken at the sampletaking devices 16, 18.

In an alternative embodiment (not represented in FIG. 1), the liftingassembly 26 can comprise permanent magnet elements in addition to or asan alternative to the lifting coils 28, 30. Preferably, two ring-shapedpermanent magnets, arranged axially at a distance from one another, arearranged in each case around the levitation element 12, located betweenwhich, at the levitation part 12, is the lifting magnet element 32. Thering-shaped permanent magnet elements are in this situation preferablyopposite magnetised. A hybrid lifting assembly, with lifting coils andpermanent magnets, is disclosed, for example, in WO 2007/065603 A1.Reference is expressly drawn to this with regard to the arrangement andformation of the permanent magnets and the lifting coils in relation toone another.

FIG. 6 shows a further example of such a hybrid lifting assembly, with,for example, two lifting coils 28, 30, and two permanent magnets 27, 29,with which the field strengths are preferably configured in such a waythat the weight force of the levitation part 12 is already fullycompensated by the lifting force of the permanent magnet elements 27,29. In the event of weight changes, for example due to samples on thesample-taking devices 16,18 in FIG. 1, the additional weight forcederiving from this can then be compensated by the lifting coils 28, 30.

In a further alternative arrangement (not represented), no lifting coilsare provided for, but, by means of two magnet rings arranged at adistance from one another, as described heretofore, a purely passivemagnetic bearing is formed. In this case, the sensor 24 is also notpresent, and no active position regulation takes place; instead, thelevitation part 12 can, for example, be coupled to an external weighingcell.

The principle structure of a levitation arrangement as in FIG. 1, aswell as details of its operation are described in WO 2007/065608 A1, towhich reference should expressly be made in this respect. Accordingly, amore detailed description of the levitation function and its use as alevitation weighing scales will not be included. Instead, a number ofimportant aspects of the structure of the magnetic levitation assembly10 will be explained.

While the position of the levitation part 12 inside the magneticlevitation assembly 10 in the example represented in the verticaldirection is, for example, actively regulated by the electromagneticlifting assembly 26 (or, in the alternative embodiment described but notrepresented, the position of the levitation part in the verticaldirection can also be held by a passive magnetic bearing), the bearings20, 22 are provided in order to centre the levitation part 12 on alongitudinal middle axis. The bearings 20, 22 are, as can be seen fromthe following detailed description, magnetic bearings, which hold thelevitation part 12 touch-free on the axis A. By way of the arrangementof two bearings 20, 22 at a distance from each other and, as shown,above and below the lifting assembly 26, good stabilizing of thelevitation part 12 is achieved. In conjunction with the continuous rigidceramic rod 14, the bearings 20, 22 enable incorrect positioning such ashorizontal displacements or oblique settings to be avoided.

FIG. 2 shows a bearing 20 in a side view; in FIG. 3 the bearing 20 isrepresented in a view from above, with a cross-section though thelevitation part 12 along the plane B.B in FIG. 2. As can be seen fromthe drawings, the bearing 20 comprises on the stationary side fourvertical magnet assemblies 34, 36, 38, 40 above one another, with acontinuous middle opening 42, in which the rod 14 of the levitation part12 is accommodated.

Arranged in ring fashion around the rod 12 is a cylindrical ring-shapedelement 44 made of diamagnetic material, such as graphite. Thediamagnetic element 44, in the example shown is longer than the bearing20, and extends through the magnet assemblies 34, 36, 38, 40. In analternative embodiment (not shown), the diamagnetic element is axiallysubstantially shorter than shown, in particular shorter than the axialdistance interval of the middle planes of two adjacent magnet assemblies34, 36, 38, 40.

The magnet assemblies 34, 36, 38, 40, of which the uppermost magnetassembly 34 can be seen in FIG. 3, are composed of magnetic segmentelements 46. These are arranged in such a way that a powerful quadrupolemagnetic field takes effect in the interior region 42.

In the example represented, the magnetic segment elements 46 form aHalbach array. With the arrangement represented, with eight segments,each of the magnet assemblies 34, 36, 38, 40 comprises eight magneticsegments 46 with trapezoidal cross-section. The magnetic segmentelements 46 are arranged immediately next to one another, such that theyform a ring around the longitudinal middle axis A, wherein each magneticsegment element 46 covers an angle region of 45° around the axis A.

The magnetizing direction of the magnetic segment elements 46 differs inthis situation, as shown in FIG. 3, between magnetic segment elements 46arranged next to one another in such a way that a rotating magnetizingis produced along the ring which is formed from these. For this purpose,the magnetic segment elements 46 comprise different types, namelymagnetic segment elements 46 a, 46 c with radial magnetizing, andmagnetic segment elements 46 b, with tangential magnetizing. Theradially magnetized magnetic segment elements 46 a, 46 c are magnetizedradially opposed to one another, i.e. some comprise an inner south pole,and the others an inner north pole. The tangentially magnetized magneticsegment elements 46 b are identical, but, as represented, are arrangedin two different rotation positions.

Magnetic segment elements 46 a, 46 b arranged in each case next to oneanother are of different types (radial/tangential magnetizing) andexhibit opposing magnetizing directions. Magnetic segment elements 46,in each case opposite one another, are of the same type(radial/tangential magnetizing), and likewise exhibit magnetizingdirections which are opposed, i.e. rotated by 180° in the plane. As aresult, a quadrupole magnetic field is produced in the free inner region42 in a middle plane (represented as the plane C.C in FIG. 2).

A corresponding field distribution in the plane is representedschematically in FIG. 4. In this situation, a minimum field strength iscreated on the longitudinal middle axis A in the centre of the plane,such that the diamagnetic element 44 is centred at the rod 14 of thelevitation part 12.

In the preferred arrangement, none of the magnetic segment elements 46exhibits an axial magnetizing, such that no magnetic field componentsare present in the axial direction in the middle plane being consideredin each case. Accordingly, a force effect is incurred on the diamagneticelement exclusively in the transverse direction but not in the axialdirection. For example, with the use of the bearing in a levitationweighing scale, a falsification of the measurement result is thereforeavoided.

It has transpired, however, that in the event of deflections of thediamagnetic element 44 out of the longitudinal middle axis A, the sameresetting forces do not take effect at all points of the interior space42. As can be seen from FIG. 4, magnetic field axes M can be definedbetween the four poles of the magnetic field in the middle plane of themagnet assembly 34. As has been shown, with a deflection along the axesM, the diamagnetic element 44 is set back to a lesser amount on the axisA than with a deflection in other directions.

Accordingly, the bearing 20 is configured with the four magnetassemblies 34,36, 38, 40 next to one another along the axis A in such away that magnetic segment elements 34, 36, 38, 40 arranged adjacent toone another are provided not with the same magnetic orientation butrotated towards one another.

In FIG. 5 this is shown schematically in an exploded representation oftwo magnet assemblies 34, 36 arranged next to one another on the axis A.In this situation, for better understanding, the magnet assemblies 34,36 are represented at a distance from one another, while, as can be seenfrom FIG. 2, they are preferably arranged axially directly next to oneanother.

As can be seen from FIG. 5, the rings of both magnet assemblies 34, 36,formed from the respective magnetic segment elements 46, exhibit in eachcase the same sequence of different magnetizings, but the second magnetassembly 36, represented on the right in FIG. 5, is rotated in aclockwise direction in relation to the magnet assembly 34, representedon the left, by a magnetic segment element 46 about the axis A. In theplanes of the magnet assemblies 34, 36, represented in each case in FIG.5 by dotted lines, there is accordingly the same field distribution ineach case in the inner region 42 as in FIG. 4, but rotated against oneanother by 45° about the axis A. In a view along the axis A, therespective field axes M of the magnetic fields taking effect in theplanes of the magnet assemblies 34, 36, are therefore not flush, butoffset against one another by 45°.

From this is derived a particularly good centring, due to the forceeffect of the two magnet assemblies 34, 36, provided next to oneanother, on the diamagnetic element 44 passing through.

In the example shown, the four magnet assemblies 34, 36, 38, 40 are ineach case rotated by the angle region of a magnetic segment element 46,i.e. by 45°, against one another about the axis A. As a result, themagnet assemblies are flush, such that a simple structure is formed. Dueto the offset of the respective magnetic fields in the middle planes,the diamagnetic element 44, and therefore the rod 14 of the levitationpart 12, is well centred in the bearing 20, wherein, with deflection inthe direction of the field axes M, a resetting and centring also takeplace.

However, with a rotation by 45° of magnet assemblies 34, 36, 38, 40arranged in each case next to one another, a flush arrangement of thefield axes is produced between the first and third magnet assemblies 34,38, as well as between the second and fourth magnet assemblies 36, 40. Astill better centring is achieved with an arrangement in which the fieldaxes M of all four magnet assemblies 34, 36, 38, 40 are in each notflush in pairs, for example with a rotation towards one another in eachcase of 20°-25° of magnet assemblies 34, 36, 38, 40 arranged next to oneanother.

The lower magnetic bearing 22 of the magnetic levitation assembly 10(FIG. 1) is of the same structure as the upper magnetic bearing 20. Inboth magnetic bearings 20, 22 in each case four magnet assembliesgenerate in each case quadrupole magnetic fields rotated against oneanother, by means of which the diamagnetic elements 44 are centred onthe longitudinal axis A.

The diamagnetic elements 44 of both bearings 20, 22 are in thissituation configured as ring elements or as circular cylindricalelements with middle boreholes, and are arranged about the continuousrod 14 of the levitation part 12. The lifting magnet element 32, and theindex element 48 of the sensor 24, secured to the levitation part, arealso in each case configured as ring-shaped or cylindrical respectively,with a middle borehole and arranged around the rod 14. In this way, therespective elements 32, 44, 48 can in each case be positioned exactly atthe levitation part, and, due to the continuous rod 14, are sufficientlyrigid to exclude deformations.

The explanation heretofore of the exemplary embodiment from FIGS. 1 to 5is to be understood as only an example and not restrictive.Modifications in relation to the elements and arrangements shown arepossible. For example, a magnetic bearing 20, 22 can exhibit a deviatingnumber of magnet assemblies 34, 36, 38, 40, for example only two magnetassemblies rotated against one another, or more than the four magnetassemblies 34, 36, 38, 40 shown. The number of magnetic segment elements46 can also deviate, as can the rotation angle of two magnet assembliesarranged next to one another. The lifting assembly 26 may have anothercoil arrangement, as well as, optionally, one or more permanent magnetelements in addition to or instead of the lifting coils.

As well as the use of the magnetic levitation assembly 10 as magneticlevitation weighing scales with sample taking devices 16, 18 as shown inFIG. 1, other uses are also possible. The magnetic levitation assembly10 can be used universally as a measuring cell or highly sensitive forcesensor for vertical forces, for example for the measurement of density,surface tension, flow, vapour pressure, viscosity, etc. FIG. 6 shows,for example, a magnetic levitation assembly 50 with the structuredescribed heretofore, with which the levitation part 12 is arranged in atube 52. As a deviation from the structure shown in FIG. 1, in this casethe lifting assembly 26 is provided, in addition to the lifting coils28, 30, with ring-shaped permanent magnet elements 27, 29, themagnetizing of which is dimensioned as dead load compensation, in such away that it compensates for the weight force of the levitation part 12.Such a hybrid lifting assembly can also be used for other embodiments.

By detection of the forces, it is possible for a measurement to becarried out simultaneously of the flow speed and the density of themedium flowing in the tube 52. As shown in FIG. 7, two magneticlevitation assemblies 54, 56 can be provided at vertical sections of thesame pipe, such that, with joint measurement, weight forces can beeasily compensated. By the addition of the forces measured, withidentically configured levitation parts, it is possible for the densityto be measured, and by subtraction simultaneously of the flow force.

1. (canceled)
 2. A measuring device including a magnetic levitation assembly, the magnetic levitation assembly comprising: a bearing including a first magnet assembly and a second magnet assembly disposed adjacent to the first magnet assembly, the first magnet assembly for generating a first quadruple magnetic field in a first plane, and the second magnet assembly for generating a second quadrupole magnetic field in a second plane that is parallel to the first plane, wherein the first and second quadrupole magnetic fields define a longitudinal axis perpendicular to the parallel planes; and a diamagnetic element disposed along the longitudinal axis defined by the bearing, wherein the second quadrupole magnetic field is rotated about the longitudinal axis, relative to the first quadrupole magnetic field, for stabilizing the diamagnetic element for movement along the longitudinal axis.
 3. The measuring device of claim 2 wherein the second quadrupole magnetic field is rotated about the longitudinal axis by other than a whole-number multiple of 90°.
 4. The measuring device of claim 3 wherein the second quadrupole magnetic field is rotated about the longitudinal axis by an angle in a range of 5° to 85°.
 5. The measuring device of claim 3 wherein the second quadrupole magnetic field is rotated about the longitudinal axis to maximize the stabilizing effect of the first and second quadrupole magnetic fields.
 6. The measuring device of claim 2 wherein the first magnet assembly comprises a plurality of magnetic segment elements for generating the first quadruple magnetic field.
 7. The measuring device of claim 6 wherein the first and second magnet assemblies have the same configuration of magnetic segment elements.
 8. The measuring device of claim 2 further comprising a second bearing including a third magnet assembly and a forth magnet assembly disposed adjacent to the third magnet assembly, wherein the second bearing is spaced from the first bearing along the longitudinal axis.
 9. The measuring device of claim 8 further comprising a lifting assembly disposed along the longitudinal axis between the first and second bearings.
 10. A measuring device including a magnetic levitation assembly, the magnetic levitation assembly comprising: a bearing including a first magnet assembly and a second magnet assembly disposed adjacent to the first magnet assembly, the first magnet assembly for generating a first magnetic field in a first plane, and the second magnet assembly for generating a second magnetic field in a second plane that is parallel to the first plane, wherein the first and second magnetic fields define a longitudinal axis perpendicular to the parallel planes; and a diamagnetic element disposed along the longitudinal axis defined by the bearing, wherein the second magnetic field is rotated about the longitudinal axis, relative to the first magnetic field, for stabilizing the diamagnetic element for movement along the longitudinal axis.
 11. The measuring device of claim 10 wherein the first magnetic field is a quadrupole magnetic field. 